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Ion Implantation and Synthesis of Materials - Studium

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4 Cross-Section4.1 IntroductionIn Chap. 3 we derived equations describing the kinematics <strong>of</strong> binary elastic collisions.These equations enable us to calculate the amount <strong>of</strong> energy-transferred to atarget atom in a collision when the scattering angle <strong>of</strong> the projectile or the targetatom is known. Conversely, we could calculate the scattering angle if the amount<strong>of</strong> energy loss in the collision was known.In Chap. 4 we will examine the probability <strong>of</strong> ion–solid scattering events. Duringion irradiation <strong>and</strong> ion implantation experiments, many ions or energetic particlesinteract with many target nuclei. Due to the large number <strong>of</strong> interactions, thequestions <strong>of</strong> how much energy will be transferred in a collision or what the scatteringangle will be must be answered using statistics <strong>and</strong> probability. The differentialcross-section is the fundamental parameter that we will develop. It gives ameasure <strong>of</strong> either the probability <strong>of</strong> transferring energy T in the range between T<strong>and</strong> T + dT to a target atom, or <strong>of</strong> the probability <strong>of</strong> scattering a projectile intosome angle between θ c <strong>and</strong> θ c + dθ c . The differential cross-section has units <strong>of</strong>area, typically centimeters squared. The differential cross-section integrated overall angles is the total cross-section, <strong>of</strong>ten referred to simply as the cross-section.The differential cross-section will become an important parameter in describingion ranges in solids <strong>and</strong> radiation damage, both <strong>of</strong> which will be discussed later inthis book. The differential cross-section depends strongly on the form <strong>of</strong> the interatomicpotential.4.2 Scattering Cross-SectionIn ion–solid interactions, it is customary to describe the number <strong>of</strong> particles scatteredthrough different angles, θ c , in terms <strong>of</strong> a quantity called the angular differentialscattering cross-section. Imagine the experiment depicted in Fig. 4.1, wherea beam <strong>of</strong> ions is incident on a thin foil <strong>and</strong> is scattered into a detector <strong>of</strong> area ∆aat a polar angle between θ c <strong>and</strong> θ c + dθ c . Each <strong>of</strong> the ions in the incident37

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